WAVELENGTH OF THE CONSTITUENT
COLOURS OF A COMPOSITE LIGHT USING DIFFRACTION GRATING AND SPECTROMETER
To
find the wavelength of the constituent colours of a composite light using
diffraction grating and spectrometer.
Spectrometer,
mercury vapour lamp, diffraction grating, grating table, and spirit level.
λ=
sinθ/ nN Å
where,
λ
→ Wavelength of the constituent colours of a composite light (Å)
N
→ Number of lines per metre length of the given grating (No unit) (the value of
N for the grating is given)
n
→ Order of the diffraction (No unit)
θ
→ Angle of diffraction (degree)
·
Eye-piece: The eye-piece of the
telescope is adjusted so that the cross-wires are seen clearly.
·
Slit: The slit of the collimator is
adjusted such that it is very thin and vertical.
·
Base of the spectrometer: The base of
the spectrometer is adjusted to be horizontal using leveling screws.
·
Telescope: The telescope is turned
towards a distant object and is adjusted till the clear image of the distant
object is seen. Now the telescope is adjusted to receive parallel rays.
·
Collimator: The telescope is brought in
line with the collimator. Collimator is adjusted until a clear image of the
slit is seen in the telescope. Now the collimator gives parallel rays.
·
Grating table: Using a spirit level, the
grating table is adjusted to be horizontal with the three leveling screws
provided in the grating table.
·
The slit is illuminated with a composite
light (white light) from mercury vapour lamp.
·
The telescope is brought in line with
the collimator. The vertical cross-wire is made to coin-cide with the image of
the slit (Figure (a)1).
·
The vernier disc alone is rotated till
the vernier scale reads 00 - 1800 and is fixed. This is the reading for the
direct ray.
·
The telescope is then rotated
(anti-clockwise) through an angle of 900 and fixed (Figure (a)2).
·
Now the plane transmission grating is
mounted on the grating table.
·
The grating table alone is rotated so
that the light reflected from the grating coincides with vertical cross-wire of
the telescope. The reflected image is white in colour (Figure (a)3).
·
Now the vernier disc is released. The
vernier disc along with grating table is rotated through an angle of 450 in the
appropriate direction such that the light from the collimator is incident
normally on the grating (Figure (a)4).
·
The telescope is released and is brought
in line with the collimator to receive central direct image. This undispersed
image is white in colour.
·
The diffracted images of the slit are
observed on either side of the direct image.
·
The diffracted image consists of the
prominent colours of mercury spectrum in increasing order of wavelength.
·
The telescope is turned to any one side
(say left) of direct image to observe first order dif-fracted image.
·
The vertical cross-wire is made to
coincide with the prominent spectral lines (violet, blue, yellow and red) and
the readings of both vernier scales for each case are noted.
·
Now the telescope is rotated to the
right side of the direct image and the first order image is observed.
·
The vertical cross-wire is made to
coincide with the same prominent spectral lines and the readings of both
vernier scales for each case are again noted.
·
The readings are tabulated.
·
The difference between these two
readings gives the value of 2θ for the particular spectral line.
·
The number of lines per metre length of
the given grating N is noted from the grating.
·
From the values of N, n and θ, the wave
length of the prominent colours of the mercury light is determined using the
given formula.
To
find the wave length of prominent colours of the mercury spectrum
(i)
For blue, λ= sinθ/ nN ,
(ii)
For green, λ= sinθ / nN
(iii)
For yellow, λ= sinθ / nN ,
(iv)
For red, λ= sinθ / nN
1.
The wavelength of blue line = ---------------- m
2.
The wavelength of green line = ------------------ m
3.
The wavelength of yellow line = ---------------- m
4.
The wavelength of red line = ---------------- m
i)
Once initial adjustments are done, spectrometer should not be disturbed.
ii)
Total reading TR = MSR + (VSC × LC)
Where
MSR
→ Main Scale Reading
VSC
→ Vernier Scale Coincidence
LC
→ Least count (= 1′)
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